Abstract: A resonating optical amplifier includes a laser pump cavity defined by a first mirror and a second mirror with a laser pump gain medium configured within a first portion of the laser pump cavity and a Raman amplifier within a second portion of the laser pump cavity. A circulating pump-laser light is introduced to the laser pump gain medium forming a pump signal that is configured to bi-directionally propagate along a beam path within the laser pump cavity. The Raman amplifier is positioned in line with the beam path of the pump signal and operable to impart gain on a seed pulse. The seed pulse and the pump signal are co-aligned and linearly polarized.

Abstract: A high brightness, wavelength-adjustable, deep-UV-C light source identifies, neutralizes, and validates the absence of one or more pathogens. An optical source using a Raman-based nonlinear optical amplification process converts low brightness continuous wave (CW) and Quasi-CW pump light into high brightness and high peak power optical UV-C radiation at a specific wavelength, pulse duration, repetition rate, and optical bandwidth for targeted pathogen identification, neutralization, and absence validation. A tunable Raman-based output operates at a wavelength between 400 nm and 460 nm, which is employed for Raman spectroscopic pathogen detection, and which is frequency doubled to the Deep-UV-C (DUV-C) spectral region of between 200 nm to 230 nm for fluorescence detection of potential pathogens.

Abstract: The invention includes a device for amplifying light having a pumping resonator and a Raman resonator that share an output mirror and are divided by an interior mirror. A pumping beam is directed though a gain medium in each resonator. A seed signal is directed into the Raman resonator, which is configured to contain cascaded Raman-shifted signals generated through the interaction of the pumping beam, seed signal, and gain medium, and to transmit a selected Raman-shifted signal as optical output. Also disclosed is a method of amplifying light using a Raman resonator that partially overlaps a pump resonator. A pumping beam is directed through a pump gain medium and a Raman gain medium and generates cascading Raman-shifted signals within the Raman resonator. A seed signal is used to shape the temporal profile, and improve the coherence, of the Raman-shifted signals.

Abstract: A high brightness, wavelength-adjustable, deep-UV-C light source identifies, neutralizes, and validates the absence of one or more pathogens. An optical source using a Raman-based nonlinear optical amplification process converts low brightness continuous wave (CW) and Quasi-CW pump light into high brightness and high peak power optical UV-C radiation at a specific wavelength, pulse duration, repetition rate, and optical bandwidth for targeted pathogen identification, neutralization, and absence validation. A tunable Raman-based output operates at a wavelength between 400 nm and 460 nm, which is employed for Raman spectroscopic pathogen detection, and which is frequency doubled to the Deep-UV-C (DUV-C) spectral region of between 200 nm to 230 nm for fluorescence detection of potential pathogens.

Abstract: A resonating optical amplifier includes a laser pump cavity defined by a first mirror and a second mirror with a laser pump gain medium configured within a first portion of the laser pump cavity and a Raman amplifier within a second portion of the laser pump cavity. A circulating pump-laser light is introduced to the laser pump gain medium forming a pump signal that is configured to bi-directionally propagate along a beam path within the laser pump cavity. The Raman amplifier is positioned in line with the beam path of the pump signal and operable to impart gain on a seed pulse. The seed pulse and the pump signal are co-aligned and linearly polarized.

Abstract: The present invention relates to the conversion of flue gas to valuable products, in particular to the conversion of carbon dioxide in flue gas to liquid fuels and valuable carbons in a carbon negative manner.

Abstract: Molecular precursor compounds, processes and compositions for making Zn-Group 13 mixed oxide materials including ABIZO, AIZO and BIZO, by providing inks comprising a molecular precursor compound having the empirical formula AlaInbBdZn(OROR)3(a+b+d)+2, and printing or depositing an ink in a film on a substrate. The printed or deposited film can be treated to convert the molecular precursor compounds to a material.

Abstract: Molecular precursor compounds, processes and compositions for making Zn-Group 13 mixed oxide materials including ABGZO, AGZO and BGZO by providing inks comprising a molecular precursor compound having the empirical formula AlaGacBdZn(OROR)3(a+C+d)+2, and printing or depositing an ink as a film on a substrate. The printed or deposited film can be treated to convert the molecular precursor compounds to a material.

Abstract: Molecular precursor compounds, processes and compositions for making Zn-Group 13 mixed oxide materials including ABIGZO, AIGZO and BAIZO, by providing inks comprising a molecular precursor compound having the empirical formula AlaInbGacBdZn(OROR)3(a+b+c+d)?2, and printing or depositing an ink on a substrate. The printed or deposited film can be treated to convert the molecular precursor compounds to a material.

Abstract: Molecular precursor compounds, processes and compositions for making Zn-Group 13 mixed oxide materials including IZO, GZO, AZO and BZO, by providing inks comprising a molecular precursor compound having the formula MAaZn(OROR)3a+2, and printing or depositing the inks on a substrate. The printed or deposited ink films can be treated to convert the molecular precursor compounds to a material.

Abstract: A laser amplifier system is presented including a pump regenerative amplifier. The amplifier generally has a cavity defined by a pair of end cavity mirrors between which an amplified pump pulse oscillates. The amplifier also includes an interaction cell with a tunable gain medium amplifies laser pulses (e.g., Raman gain). The interaction cell may be positioned within the pump amplifier cavity and an input pulse may be injected into the cavity of the amplifier to transit through the tunable gain medium of the interaction cell. A pump pulse transfers energy via interaction with the input pulse (e.g., Raman interaction) as the pulses counter-propagate through the gain medium of the interaction cell. Amplification of output laser pulses, however, is generally achieved according to the wavelength of the pump laser pulses thereby providing a wavelength dependent, or “tunable”, means for amplifying laser pulses.

Abstract: Processes for making a solar cell by depositing various layers of components on a substrate and converting the components into a thin film photovoltaic absorber material. Processes of this disclosure can be used to control the stoichiometry of metal atoms in making a solar cell for targeting a particular concentration and providing a gradient of metal atom concentration. A selenium layer can be used in annealing a thin film photovoltaic absorber material.

Abstract: Processes for making a thin film solar cell on a substrate by providing a substrate coated with an electrical contact layer, depositing an ink onto the contact layer of the substrate, wherein the ink contains an alkali ion source compound suspended or dissolved in a carrier along with photovoltaic absorber precursor compounds, and heating the substrate. The alkali ion source compound can be MalkMB(ER)4 or Malk(ER). The processes can be used for CIS or CIGS.

Abstract: Processes for making a solar cell by depositing various layers of components on a substrate and converting the components into a thin film photovoltaic absorber material. Processes of this disclosure can be used to control the stoichiometry of metal atoms in making a solar cell for targeting a particular concentration and providing a gradient of metal atom concentration. A selenium layer can be used in annealing a thin film photovoltaic absorber material.

Abstract: This invention relates to methods for materials using compounds, polymeric compounds, and compositions used to prepare semiconductor and optoelectronic materials and devices including thin film and band gap materials. This invention provides a range of compounds, polymeric compounds, compositions, materials and methods directed ultimately toward photovoltaic applications, transparent conductive materials, as well as devices and systems for energy conversion, including solar cells. This invention further relates to thin film AIGS, AIS, and AGS materials made by a process of providing one or more polymeric precursor compounds or inks thereof, providing a substrate, depositing the compounds or inks onto the substrate; and heating the substrate at a temperature of from about 20° C. to about 650° C.

Abstract: This invention relates to compounds, polymeric compounds, and compositions used to prepare semiconductor and optoelectronic materials and devices including thin film and band gap materials. This invention provides a range of compounds, polymeric compounds, compositions, materials and methods directed ultimately toward photovoltaic applications, transparent conductive materials, as well as devices and systems for energy conversion, including solar cells. In particular, this invention relates to polymeric precursor compounds and precursor materials for preparing photovoltaic layers. A compound may contain repeating units {MB(ER)(ER)} and {MB(ER)(ER)}, wherein MA is Ag, each MB is In or Ga, each E is S, Se, or Te, and each R is independently selected, for each occurrence, from alkyl, aryl, heteroaryl, alkenyl, amido, silyl, and inorganic and organic ligands.

Abstract: This invention relates to compounds and compositions used to prepare semiconductor and optoelectronic materials and devices. This invention provides a range of compounds, compositions, materials and methods directed ultimately toward photovoltaic applications, as well as devices and systems for energy conversion, including solar cells. In particular, this invention relates to molecular precursor compounds, precursor materials and methods for preparing photovoltaic layers and thin films thereof.

Abstract: Processes for making a photovoltaic layer on a substrate by depositing a first layer of an ink onto the substrate, wherein the ink contains one or more compounds having the formula MB(ER)3, wherein MB is In, Ga, or Al, E is S or Se, and depositing a second layer of one or more copper chalcogenides or a CIGS material.

Abstract: The various laser architectures described herein provide increased gain of optical energy as well as compensation of optical phase distortions in a thin disk gain medium. An optical amplifier presented herein provides for scalable high energy extraction and gains based on a number of passes of the signal beam through a gain medium. Multiple, spatially separate, optical paths may also be passed through the same gain region to provide gain clearing by splitting off a small percentage of an output pulse and sending it back through the amplifier along a slightly different path. By clearing out the residual gain, uniform signal amplitudes can be obtained.

Abstract: Provided is a laser dazing apparatus shaped as a pistol having an encasement formed by a elongated barrel (114) joined to a handle (117), together forming an encasement. The barrel (114) has a forward end and a rear end, and the handle (117) is connected to the barrel (114) towards the barrel's rear end. The barrel encasement (114) also includes an adapter ring (111) with a focusing fixture (112) for controlling divergence of radiation produced by the device. The apparatus also includes various indicators, a laser generator, a least one battery for electrical power, and a plurality of control circuits controlling the laser generation device, battery, indicators and switches. The apparatus also includes a focus range adjuster (105).